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<article article-type="research-article" dtd-version="1.3" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xml:lang="en"><front><journal-meta><journal-id journal-id-type="publisher-id">mrisel</journal-id><journal-title-group><journal-title xml:lang="en">Magnetic Resonance in Solids</journal-title><trans-title-group xml:lang="ru"><trans-title>Magnetic Resonance in Solids</trans-title></trans-title-group></journal-title-group><issn pub-type="epub">2072-5981</issn><publisher><publisher-name>Kazan Federal University</publisher-name></publisher></journal-meta><article-meta><article-id custom-type="elpub" pub-id-type="custom">mrisel-211</article-id><article-categories><subj-group subj-group-type="heading"><subject>Research Article</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="ru"><subject>Статьи</subject></subj-group></article-categories><title-group><article-title>EPR and evidence for two structural nonequivalent states  of Tl2+(II) paramagnetic centers near noncentral positions in Rb2SO4 and Cs2SO4 crystals</article-title><trans-title-group xml:lang="ru"><trans-title></trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="western" xml:lang="en"><surname>Mamin</surname><given-names>G. V.</given-names></name></name-alternatives><bio xml:lang="en"><p>Kremlevskaya, 18, Kazan 420008</p></bio><email xlink:type="simple">george.mamin@kpfu.ru</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="western" xml:lang="en"><surname>Efimov</surname><given-names>V. N.</given-names></name></name-alternatives><bio xml:lang="en"><p>Kremlevskaya, 18, Kazan 420008</p></bio><email xlink:type="simple">vladimir.efimov@kpfu.ru</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff xml:lang="en" id="aff-1"><institution>Kazan State University</institution><country>Russian Federation</country></aff><pub-date pub-type="collection"><year>1999</year></pub-date><pub-date pub-type="epub"><day>21</day><month>01</month><year>2024</year></pub-date><volume>3</volume><issue>2</issue><fpage>1</fpage><lpage>8</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; Mamin G.V., Efimov V.N., 2024</copyright-statement><copyright-year>2024</copyright-year><copyright-holder xml:lang="ru">Mamin G.V., Efimov V.N.</copyright-holder><copyright-holder xml:lang="en">Mamin G.V., Efimov V.N.</copyright-holder><license xml:lang="ru" license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>Данная работа распространяется под лицензией Creative Commons Attribution 4.0.</license-p></license><license xml:lang="en" license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>This work is licensed under a Creative Commons Attribution 4.0 License.</license-p></license></permissions><self-uri xlink:href="https://www.mrsej.ru/jour/article/view/211">https://www.mrsej.ru/jour/article/view/211</self-uri><abstract><p>The EPR spectrum temperature dependence of Tl2+(II) paramagnetic centers in Rb2SO4, Cs2SO4 crystals have been investigated. At 100K&gt;T&gt;40K the local symmetry of Tl2+(II) paramagnetic centers is C2. The broadening and doubling of EPR spectrum lines with decreasing of T&lt;40K were observed. The angular dependence of lines positions indicate that two structural nonequivalent positions of Tl2+(II) paramagnetic center exist at T&lt;20K. The measurement of dielectric constant of crystals displayed the absence of phase transition in this temperature range. The transformation of EPR spectrum is explained by motion ofTl2+(II) paramagnetic center between two structural nonequivalent states arising near noncentral positions. Parameters of the potential have been extracted by fitting of the temperature dependence of EPR spectrum. Two nonequivalent states are possible due to large difference between ionic radius of Tl2+(II) and Rb+, Cs+.</p></abstract><kwd-group xml:lang="en"><kwd>electron paramagnetic resonance</kwd><kwd>noncentral ions</kwd><kwd>local dynamics</kwd></kwd-group><funding-group><funding-statement xml:lang="en">The work was in part supported by the Russian State Foundation for Basic Research, Grant No 98-02-18037.</funding-statement></funding-group></article-meta></front><back><ref-list><title>References</title><ref id="cit1"><label>1</label><citation-alternatives><mixed-citation xml:lang="ru">Efimov V.N., Mamin G.V. Mod. Phys. Lett. B 11, 579 (1997)</mixed-citation><mixed-citation xml:lang="en">Efimov V.N., Mamin G.V. Mod. Phys. Lett. B 11, 579 (1997)</mixed-citation></citation-alternatives></ref><ref id="cit2"><label>2</label><citation-alternatives><mixed-citation xml:lang="ru">Mamin G.V., Efimov V.N. Mod. Phys. Lett. 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